Description

A nanometre-scale superconducting electrode connected to a reservoir via a Josephson junction constitutes an artificial two-level electronic system: a single-Cooper-pair box. The two levels consist of charge states (differing by 2e, where e is the electronic charge) that are coupled by tunnelling of Cooper pairs through the junction. Although the two-level system is macroscopic, containing a large number of electrons, the two charge states can be coherently superposed. The Cooper-pair box has therefore been suggested as a candidate for a quantum bit or ‘qubit’—the basic component of a quantum computer.

Figure

Motivation

The original “artificial atom” formed in a superconducting circuit. Because of its sensitivity to charge noise, alternative qubit approaches that offer some immunity to charge noise were sought after.

References

Linked Papers

Seed Metadata

  • date_published: 1999-04-29

Physics

The Cooper pair box Hamiltonian:

Operating in the charge regime , the qubit states are charge states and differing by one Cooper pair. At the charge degeneracy point , the two lowest states are split by . Gate voltage tunes , controlling the qubit transition frequency. Highly sensitive to charge noise at generic operating points.

  • transmon — descendant operating in for charge noise immunity
  • fluxonium — inductive shunt alternative
  • blochnium — quasicharge regime

Key Metrics

MetricValueNotesFidelity reference
Qubit coherence ~1–10 μsLimited by charge noiseNakamura et al. 1999
Qubit coherence ~0.5–5 μsAt sweet spot ()Vion et al. 2002
Gate fidelity (1Q)~99%Voltage-pulse drivenVion et al. 2002
Gate fidelity (2Q)~95%Capacitive couplingYamamoto et al. 2003
Gate time (1Q)~1–10 nsFast voltage pulses
Gate time (2Q)~10–50 ns
Readout fidelity~90–95%Probe junction or SETVion et al. 2002
Qubit footprint~1 × 1 μm²Very compact
Operating temperature20–50 mKDilution refrigerator
ConnectivityFixed capacitiveNearest-neighbor